Generators of relations for annihilating fields
| dc.creator | Primc, Mirko | |
| dc.date | 2002-04-23 | |
| dc.date.accessioned | 2026-07-07T04:48:01Z | |
| dc.date.available | 2026-07-07T04:48:01Z | |
| dc.description | For an untwisted affine Kac-Moody Lie algebra $\tilde{\mathfrak g}$, and a given positive integer level $k$, vertex operators $x(z)=\sum x(n)z^{-n-1}$, $x\in\mathfrak g$, generate a vertex operator algebra $V$. For the maximal root $θ$ and a root vector $x_θ$ of the corresponding finite-dimensional $\mathfrak g$, the field $x_θ(z)^{k+1}$ generates all annihilating fields of level $k$ standard $\tilde{\mathfrak g}$-modules. In this paper we study the kernel of the normal order product map $r(z)\otimes Y(v,z)\mapsto :r(z) Y(v,z):$ for $v\in V$ and $r(z)$ in the space of annihilating fields generated by the action of $\tfrac{d}{dz}$ and $\mathfrak g$ on $x_θ(z)^{k+1}$. We call the elements of this kernel the relations for annihilating fields, and the main result is that this kernel is generated, in certain sense, by the relation $x_θ(z)\tfrac{d}{dz}(x_θ(z)^{k+1})= (k+1)x_θ(z)^{k+1}\tfrac{d}{dz}x_θ(z)$. This study is motivated by Lepowsky-Wilson's approach to combinatorial Rogers-Ramanujan type identities, and many ideas used here stem from a joint work with Arne Meurman. | |
| dc.description | 13 pages, AMS-LaTeX | |
| dc.identifier | https://arxiv.org/abs/math/0204283 | |
| dc.identifier | http://arxiv.org/abs/math/0204283 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/63893 | |
| dc.subject | Quantum Algebra | |
| dc.subject | 17B67 | |
| dc.title | Generators of relations for annihilating fields | |
| dc.type | text |